In , the characteristic equation of a partial differential equation gives . Integration yields the characteristic coordinates
Their Jacobian determinant is , so they are valid independent coordinates. To see cancellation of the lower-order terms explicitly, first put , and . The chain rule gives
Substitution cancels the first-derivative terms, leaving . With , and , the characteristic normal form is . Integrating once in each variable gives
where are arbitrary twice continuously differentiable functions on the relevant coordinate intervals. This is a curvilinear reduction to the one-dimensional wave equation.

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